Experimental data are reported on flow regimes, gas hold-up and axial gas mixing of a gas-liquid Multi-stage Agitated Contactor (MAC), consisting of nine compartments [height, H, over diameter, D = 1; D = 0.09 m) separated by horizontal baffles with an opening of 0.04 m and with one centrally positioned impeller per compartment (12-bladed turbine disk; impeller diameter, d I = 0.03 m). For air-water and the liquid in batch, a homogeneous gas-liquid dispersion is realized with a stirring speed, N, above 15 s −1 and a superficial gas velocity, u G, below 0.12 m s −1. These boundaries are affected unfavourably by either a cocurrent or a countercurrent liquid flow. For nine combinations of three gases (air, helium and dichloro-difluoro methane) and three liquids (water, n-octane and monoethylene glycol) the gas holds-up, ε G , and the axial gas mixing were determined with the liquid in batch. Experimental conditions were varied as follows: u G , 0.01–0.09 m s −1; N, 10–36.7 s −1; liquid viscosity, η L , 0.00041–0.021 Pa s; surface tension, σ, 0.02–0.073 N m −1; liquid density, ϱ L , 684–1113 kg m −3 and gas density, ϱ G , 0.16–5.16 kg m −3. For all experiments, the residence time distribution of the gas phase could be described excellently with a Cascade of ideally mixed Tanks in series with Alternating Backflow model (CTAB model). All 85 data ε G could be correlated with an average relative deviation of 11.0% by an extension of Van Dierendoncks' empirical gas hold-up relation. The relative gas backflow (ratio between gas backflow and net gas flow) data could be correlated by a novel relation with average relative deviations of 14.5, 17.7 and 19.5% for air-water (18 data points), helium- n-octane (19 data points) and air-monoethylene glycol (12 data points) systems, respectively.
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